I studied physics for five years at CA State University-Sonoma and -San Francisco. Familiar with the wave-particle paradox, I studied with an imaginative but critical mind toward extracting nature's message from current dogma. As owner of Computer Continuum for 15 years I successfully designed and sold computer add-on circuits for robotics, A/D, DSP, etc. My past efforts and inventions span many fields: fundamental physics, bioelectromagnetics, vacuum technology, lasers and optics, automation, mechanical systems, computers and interface, alternative energy, physiological monitoring, bookbinding, home design, fine art, and music. I've been independently studying and developing experiments in fundamental physics since 1999.


spie 9570-25 Eric Reiter 2My first lecture to formal physicists spie 9570-25 Eric Reiter


Live experiment demonstrations at the Chit-Chat Cafe



With a lathe chuck on a milling machine, it can do both lathe and light mill work.  A 3/4″ tool bit is in the mill vise.

This is a fine cut on a 3.5″ aluminum disk to be used for yet another alpha-particle mortification machine.  I mean the experiment defies the idea that the atom is always a particle.  My earlier experiments have shown many ways the alpha splits like a wave.  It would need to defy the binding energy calculation to split into two deuterons or something.  Besides, I did experiments that gave two-for-one at 4 X chance, defying particle-energy conservation, in evidence of the loading theory.   The disk is the base plate for a small bell jar vacuum chamber.


Abstract for A Challenge to Quantized Absorption by Experiment and Theory

After recognizing dubious assumptions regarding light detectors, a famous beam-split coincidence test of the photon model was performed with gamma-rays instead of light. A similar test was performed to split alpha-rays. Both tests are described in detail to justify conclusions. In both tests coincidence rates greatly exceeded chance: the unquantum effect. This is a strong experimental contradiction to quantum theory. These new results are interpreted as evidence of the long abandoned accumulation hypothesis, also known as the loading theory, and draw attention to assumptions applied to key past experiments that led to quantum mechanics. The history of the loading theory is outlined. Planck’s second theory of 1911 was a loading theory. A popular incomplete version of the loading theory that convinced physics students to reject it is exposed. The loading theory is developed by identifying dubious assumptions in de Broglie’s matter-wavelength equation derivation, and re-deriving a matter-wavelength equation from the photoelectric effect equation. The loading theory is applied to the photoelectric effect, Compton effect, and charge quantization, now free of wave-particle duality. The loading theory is unlikely to apply to recent claimed success of giant molecule diffraction, and this issue is addressed. This all leads to concluding that quantized absorption is an illusion, due to quantized emission combined with newly identified properties of the matter-wave.

Please read the essay here:

Recent arguments over “Real-time single-molecule imaging of quantum interference” experiment

 Uncategorized  Comments Off on Recent arguments over “Real-time single-molecule imaging of quantum interference” experiment
May 222012

This is the interaction I had by email to the first named author.   Below is the author’s response.   What do I think of his response?  Each point was handled poorly in a typical attitude of denial.   You need to read the original paper to understand the issues.  ER


On Di, 22.05.2012, 01:54, Eric Reiter wrote:
> Dear Dr Juffmann
> Regarding your recent article, “Real-time single-molecule imaging of
> quantum interference,” I have performed calculations on your data that do
> not make sense to me.
> 1) Let’s calculate the fall of a particle. We can use (1/2)gt^2, where t
> = time = distance/velocity. For a fast particle Hfast =
> (9.8/2)(2m/340m/s)^2 = 169×10^-6 meters. For a slow particle Hslow =
> (9.8/2)( 2m/140m/s)^2= 1×10^-3 meters. Hslow – Hfast = 830 micrometers.
> But you show only 240 micrometers. Therefore the difference in falls
> should be 3.4 times larger than you show.
> 2) I used a multiple slit diffraction simulation tool to test what the
> intensity profiles should be. I found your first order fringes were a few
> times brighter than they should be for the given wavelength/slit-width and
> wavelength/slit-spacing ratios. The the tool I used is
> Though
> this tool has fewer slits than yours, I found this did not change the
> intensity ratios.
> 3) Given the dimensions of your instrument, the velocity resolution should
> cover 0.43 of the sensor plane by the following calculation: The slit
> height is 100 micrometers, and the projection to the sensor plane should
> make this 2/(2 – 0.56) larger, that is 138 micrometers at the sensor
> plane. But the sensor plane is 320 micrometers high. Since 138/320 =
> 0.43, a particle of any given velocity could land anywhere in a vertical
> segment of height that is 0.43 of the screen height. So the first order
> fringes should have been very noticably widened as the fringes descend, by
> this apparently poor velocity resolution.
> 4) In the published movies of the detector plane, the intensity profiles
> of the fringes have edges that seem to rise and fall too abruptly. Also,
> the intensity profile of each fringe, especially the central fringe, in
> the movie looks flat. Fringes should have peak-like profiles. The fact
> that the peaks appear in fig 4c is irrelevant since they are a result of
> integrating offset overlapping square shaped fringes between the dashed
> yellow lines.
> Unless I have made several silly errors, there is something going on other
> than quantum interference. Please consider a control test to eliminate
> the possibility that you are looking at a shadow pattern that has been
> magnified by a charge deflection effect at the slits. It would be very
> easy for the slits to become charged to deflect dye particles in a manner
> similar to a cylindrical lens. A simple test would be to introduce a
> voltage control wire to the slits. An even simpler test would be to shade
> half of the slit array to see if a half side of the fringe pattern
> disappears. Whether or not a focus effect was like a positive or negative
> lens, half of the fringe pattern would disappear. A focused shadow would
> explain the anomalies I point out.
> Thank you for your consideration and I hope to hear from you.
> Eric S Reiter
> Unquantum Laboratory


Dear Mr. Reiter,
concerning your considerations:
1) The equations are of course right, but our source emits molecules in
all directions. Thus a flight parabola is defined by three source, the
grating (which is only written onto a 100µm high window) and the height on
the detection plane. Thus it is wrong to simply enter the distance
source-detection plane into the calculations, since in the plane of the
grating all molecules pass at the same height.

2) Your observatin is right. The high intensity of the higher interference
orders is due to the van der Waals interaction between the molecules and
the grating wall. This is mentioned several times in our paper.

3) Please don’t forget, that also the grating is only 100µm high and that,
especially for the slow molecule, the projection is a non valid

4)I don’t agree. Regarding the high transversal coherence in our
experiment the shape of the fringes is in agreement with the theoretical

Best regards,
Thomas Juffmann


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